Light collection and distribution

ABSTRACT

A light box is designed to receive sunlight guided through optical-fibers and to divert it through optics onto a photovoltaic chip which converts sunlight into electrical energy. The optics can be arranged as a prism or a reflective surface. The chip is not integrated with the light box.

FIELD

This invention relates to light collection and distribution particularly but not exclusively in the field of photovoltaic energy conversion.

BACKGROUND

Two types of photovoltaic energy conversion technologies are in use today. One is in the form of panels, comprising of wafers of a semiconductor material that contain cells linked together to produce a unit whose size can be as large as 99 cm by 195 cm in commercial grade panels. In these types of panels, the semiconductor material that converts light to electricity is sandwiched between a structural aluminum backing material, and a top glazing from which the light (solar radiation) is incident. Silicon is the dominant semiconductor material in panels of this kind. Light incident on such panels can be from any angle; i.e., they can accept diffuse light.

The second type of photovoltaic technology uses collection optics to gather and concentrate light onto small areas of semiconductor where light-sensitive cells are fabricated. This is the basis of concentrated photovoltaic (CPV) technology, where compound semiconductor thin films synthesized from group III-V compounds are used for the light-sensitive cells. Two of its main virtues are that it uses less semiconductor material and yet has a much higher conversion efficiency of 40% in research-grade multi junction cells, compared to a typical conversion efficiency of 18-25% for silicon panels. Concentrated photovoltaic modules accept normal incidence light, and are typically provisioned with a tracking system that keeps the modules optimally aligned to the sun to consistently produce the most energy on any typical day. Unlike flat plate silicon panels, light collection optics are integrated onto CPV modules. Because of the high concentration of light incident on a cell module, there is a need to uniformly distribute incident light over the area of the solar cell chip. Such areas can range from a few square millimeters to several tens of square centimeters. Distributing light uniformly over these areas is necessary because it avoids the onset of hot or cold spots that could damage a chip. This is particularly important for large area chips (>25 mm²). The usual approach to distributing light over CPV cells is to use a truncated pyramidal glass prism that is attached (with an index-matching epoxy) to the cell. Light incident on the large surface of the prism is guided along the length of the prism by total internal reflections and emerges scrambled at the bottom of the prism, where it is attached to a solar cell. Properly dimensioned prisms can often achieve uniform light distribution over the surface of a solar cell. However, a number of issues have dogged this approach. Among them is the fact that the multiple surfaces and interfaces of the prism can cause cumulative light loses that can be significant. The second other major issue is delamination of the prisms from cells due to temperature variations. A third problem is connected to the manufacture of the prisms. Most are manufactured manually, resulting in a time consuming and costly process. Nevertheless, the inventor recognizes that CPV technology has potential for scalability in constructing large-scale power plants at low cost, if the above problems could be solved.

SUMMARY

According to one aspect of the invention there is provided a light collection housing adapted to receive light from a plurality of point light sources, the light collection housing having: at least one light transmissive region adapted to receive light beams from a plurality of point light sources; securing means for securing the light sources relative to the housing to direct their respective beams through the light transmissive regions into the housing and an optical guidance arrangement being such that the beams are guided into overlap at an exit region of the housing to form an illumination zone of substantially uniform intensity distribution.

An important premise underlying the invention is that light is often available in spatial forms and intensity distributions that are not suitable for certain applications. A case in point is light beams harnessed from sunlight. By using the light collection housing of one aspect of this invention, it is rendered possible to make use of sunlight guided in optical fibers to the housing from a harvesting location. At the harvesting location, the sunlight can be collected, focused down to a point, and coupled to a fiber waveguide for transport to a location remote from the harvesting location, where the collection housing is located. Here, when it emanates from the fiber end, it diffracts, with an angular spread related to the numerical aperture. While a fiber cable with many strands of fiber in it can deliver a lot of power, this raw power may not have the appropriate intensity distribution or the correct geometrical beam shape.

These matters can be addressed in embodiment of the invention. There is described herein an apparatus and a method for providing a uniform light distribution of the application. In one example, concentrated photovoltaic solar cells are used to illustrate the concept. This example is concerned with a method and an apparatus for uniformly distributing sunlight over solar cells chips for a more efficient photovoltaic conversion process.

In another example, the uniformly distributed light may act as a lamp.

The optical guidance arrangement of the light collection housing may comprise an inclined reflecting surface arranged to receive the beams from the point light sources and to reflect them to the illumination zone in overlap. Additionally, the light collection housing may comprise at least one microstructured diffuser at the illumination zone configured to receive the overlapping beams and adapted to spread the received light with a substantially uniform intensity distribution over an area with a defined geometrical shape.

The securing means of the light collection housing may be configured to secure the light sources in one or more arrays.

The optical guidance arrangement of the light collection housing may comprise a prism providing the reflecting surface. Alternatively, the optical guidance arrangement of the light collection housing may comprise an opaque block with a dielectric coating constituting the reflective surface.

The optical guidance arrangement of the light collection housing may comprise two inclined reflecting surfaces arranged to receive beams from respective sets of point light sources secured at opposite walls of the housing, and to reflect them in overlap to the illumination zone, and where there is at least one microstructured diffuser associated with the illumination zone. A further microstructured diffuser may be arranged in parallel with the first microstructured diffuser in the direction of the beams.

The inclined reflective surface of the light collection housing may have an angle with respect to the horizontal lower surface of the housing of 30° to 60° , optionally 45°.

The light sources of the light collection housing may be terminal ends of optical fibers. Alternatively, the light sources may be light-emitting diodes.

The light sources of the light collection housing may be each terminated with a tip that shapes its beam entering the housing.

The light collection housing may comprise a fixture which supports the light collection housing, relative to a photovoltaic component wherein the light of uniform intensity and defined geometrical shape exiting the microstructured diffuser is directed at the photovoltaic component of the same geometrical shape.

According to another aspect of the invention there is provided a method for collecting light at a housing adapted to receive light transported from a plurality of point light sources, the method comprising: receiving light beams from a plurality of light sources via at least one light transmissive region; securing the light sources relative to the housing with a securing means to direct their respective beams through the light transmissive regions into the housing; and guiding the beams into overlap at an exit region of the housing to form an illumination zone of substantially uniform intensity distribution.

The method for collecting light at a housing may comprise receiving the beams from the light sources at an inclined reflecting surface arranged to reflect them to the illumination zone in overlap. The method may additionally comprise reflecting the beams from the reflecting surface in overlap toward at least one microstructured diffuser at the illumination zone, wherein the microstructured diffuser is adapted to spread the received light with a substantially uniform intensity distribution over an area with a defined geometrical shape.

The securing means of the method for collecting light may be configured to secure the light sources in one or more arrays.

The method for collecting light may comprise receiving the beams from two sets of light sources secured at opposite walls of the housing at two inclined reflecting surfaces that reflect them in overlap to the illumination zone.

The method for collecting light may comprise directing the light of uniform intensity and defined geometrical shape exiting the microstructured diffuser at a photovoltaic component of the same geometrical shape.

When used in the context of photovoltaic conversion, the approach described in the following enables limitations in the existing approaches to be overcome. These limitations are rooted in the design philosophy of all current flat plate photovoltaic panels and concentrated photovoltaic modules. Conventional panels and modules are designed to integrate several functions of the solar-electric energy generation process into a single system. While this might appear to be a reasonable strategy, the inventor has recognized two major flaws. Technologies that involve semiconductors generally improve their performance every few years and, along the way, the cost of producing them also drops. However, the existing approach does not enable such improvement to be taken advantage of Furthermore, it is rarely possible to optimize an engineering system comprised of many components in a single shot; this is especially so if different materials or structures are integrated to form a whole. In this particular case, the light collection process and the light-to-electricity conversion process cannot be easily optimized when a single structure is used for both. The first penalty paid for integration is fewer collected photons (light particles) and a constraint in where the light-to-electricity conversion process can take place; the second penalty is a lockout on upgrades to more efficient future semiconductor devices that perform the light-to-electricity conversion process. This latter impediment is particularly severe given that solar cell devices, like other semiconductor devices, routinely see periodic improvements in their conversion efficiencies every few years.

Light collection housings described herein make it convenient, easy, and inexpensive to supply captured solar energy to separately replaceable banks of semiconductor chips.

This design makes it feasible to contemplate upgrading the performance of a photovoltaic plant every few years when improvements are made in the technology. Replacing the carrier and the bank of chips on it is relatively inexpensive compared to gutting an entire infrastructure. Furthermore, the approach guarantees that any photovoltaic plant constructed in this manner is future-proof.

A point source has a defined and homogeneous light beam aperture, having a strong illumination focus, producing a sharply defined and evenly lit luminous spot. In a point source, the area from which the light emanates must not be large, i.e. must not form an ‘extended source’, since an extended source has different characteristics that make it work without having to integrate optics to pre-shape the beam profile. The point light sources may be end-points of light transport guides used to harvest and transport sunlight. The light transport guides may take the form of optical-fibers, referred to herein as fiber-optic waveguides in some places. It will be appreciated that the terms ‘optical-fiber’ and ‘fiber-optic waveguides’ may be used interchangeably. A cable may house several optical-fibers in a protective housing. Once it is coupled to fiber-optic waveguides, sunlight can be transported safely by routing the cables from a collection location to a conversion location where the energy can be converted into electricity. The distances over which sunlight might be transported can be as short as a few tens of meters away from where it is collected, or the distances can span a city, a country or even a continent as long as most fiber absorption losses and coupling losses can be minimized.

The light transport waveguide may be capable of delivering sunlight along its length for distances of up to 1 km with minimal loss on the order of 10 dB per kilometer or less over the spectral band in which most solar energy is contained. For example, suitable light transport waveguides may be capable of transporting light rays that span the wavelength range from 350 nm to 2500 nm, which corresponds to the spectral band where most (around 95%) of solar energy reaching earth is concentrated.

By separating out the collection of the light from its use, it is possible to consider methods and structures that allow for simple upgrading of technical components of the apparatus. For example, according to embodiments described herein a light cabinet is described which has racks for accommodating light collection housings above a replaceable bank of solar cells. The solar cells are located to receive solar power from the illumination zone of housings located in the rack upon rack mountings. The solar cells can be in the form of chips whose sizes can range from a few square millimeters to several tens of square centimeters. The transported sunlight is delivered to the light cabinets via the light transport guides, and the same light transport guides can be used to distribute light over the solar cell chips. Alternatively, light transport guides can be connected together. The chips may be mounted on carriers, and both the bank of chips and the carriers on which they are mounted may be standardized to allow easy replacement of the chips (by replacing an entire chip carrier with a new one that possesses a new bank of chips).

For a better understanding of the present invention and to show how the same may be carried into effect reference will now be made by way of example to the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A shows an array of solar collector modules for harvesting sunlight at a collection location.

FIG. 1B is a sectional view through a solar collector module

FIG. 2A is an open side view of a light cabinet

FIG. 2B is front open view of a light cabinet

FIG. 2C is a detailed sectional view through an electrical conversion assembly

FIG. 2D is an expanded view of the electrical conversion assembly

FIG. 2E is a sectional view through a light box

FIG. 2F is a sectional view of a light box

FIG. 3 is an expanded view of multiple electrical conversion assemblies associated with a single rack of the cabinet

FIG. 4 is a plan view showing the coolant system placed under a chip carrier

FIG. 5 is a perspective view showing the arrangement of a chip carrier within its carrier block

FIG. 6 is a plan view of a chip carrier carrying multiple PV chips

DETAILED DESCRIPTION

The present embodiments provide an apparatus and method for providing light of a substantially uniform intensity distribution for a number of applications including, but not limited to, photovoltaic energy conversion. A particularly advantageous method of coupling sunlight from a fiber-optic cable onto a solar cell chip is described herein. The sunlight is coupled into a light box where several delivery fibers inject light into a cavity so that light from multiple fibers can mix and scatter at engineered surfaces and, optionally, at an optical diffuser attached to the surface of the light box that faces the solar cell chip. In one embodiment, the output of the diffuser may be a uniform square or rectangular shaped beam of light whose size precisely matches the size of a solar cell chip under the light box.

The first embodiment is discussed in the context of a system in which sunlight is harvested and transported using optical fibers.

FIGS. 1A and 1B illustrate a solar collection system which comprises one or more arrays 100 of solar collector modules 200. Each solar collector module is dish-shaped and acts to receive sunlight rays 204 and 205 from its upper flat or open surface and to direct that sunlight using optical components to a light receiver 210 located at the lower central region of the dish. In the described embodiments, the light receiver 210 is a fiber-optic waveguide 210. The fiber-optic waveguide 210 from each solar collector module in the array can be collected together and housed in a fiber-optic cable 401 for each array.

In the present description, the term optical-fiber is used interchangeably with fiber-optic waveguide to denote a long cylindrical silica glass core surrounded by a cladding whose index of refraction is smaller than that of the core. The cladding, in turn, is surrounded by a protective polymer coat. The entire structure is encapsulated in a hard but flexible protective outer polymer layer called the jacket. The term fiber strand is used herein to denote a single optical-fiber waveguide. The phrase ‘optical-fiber (or fiber-optic) cable’ is used to denote a tough but flexible protective thermoplastic housing with multiple optical-fibers for the purpose of light transport. ‘Super’ cables can be provided for carrying multiple cables over long distances.

The revolutionary arrangement described herein thus enables sunlight to be collected at a location where sunlight is plentiful (a collection location), and transported to a location separated from the collection location. The distance of separation could be small or large, and is limited only by the possible length of fiber-optic cables and management of absorption losses. Once coupled into fiber-optic waveguides, sunlight can be transported safely by routing the fiber-optic cables to any desirable location where the sunlight energy can be further processed or manipulated into a desired form (electrical or thermal). The distances over which sunlight might be transported can be as small as tens of meters away from where it is collected, or the distances can span a city, a country or even a continent as long as most fiber absorption losses and coupling losses can be minimized.

The examples described herein make use of a radical new approach that separates the process of harvesting sunlight from its immediate utilization or conversion to other forms of energy. Instead of the integrated approaches that have been developed in the past, the present approach separates the processes involved in solar energy harvesting and the use of that energy.

FIG. 1A shows an assembly of paraboloid solar collector modules 200 in an array 100 on a supporting surface 103 that is mounted on a pedestal 101. The pedestal 101 has a rack 105 on which the hexagonal collector array 100 is mounted. To follow the daily movements of the sun, the collector array 100 is provisioned with a two-axis, motor-driven (not shown) system for positioning and pointing the entire structure to the most optimal direction for collecting the most sunlight at any time during a sunny day. A solar tracking sensor 102 provides a control signal for driving a programmable logic controller [not shown] that controls the two-axis tracking system. Details of the two-axis tracking system and the programmable logic controller are not described further herein, because there are known systems which are currently used to control the angle of orientation of solar panels which could be adapted for this purpose. The individual collector modules can be arranged in the array in any two-dimensional geometric shape desired. However, the arrangement in this embodiment is such that the final geometric form, when looked at from a plan view, is a hexagon. This arrangement is preferred in some contexts because it is predicated on a geometric optimization principle that produces a hexagon as the ideal geometric form for the highest packing density (per unit area) for arranging dish-shaped, concave structures with circular rims, resulting in an effective coverage of about 91%.

Each collector module 200 may be designed to securely fit inside a holding substructure 103 in a manner to allow simple removal and replacement. Alternatively, a complete array of collector modules can be fabricated as a single structure which can easily be removed and replaced from the rack 105.

A single collector module 200 is shown in FIG. 1B. The collector module 200 is a hollowed-out paraboloid dish formed from an appropriately truncated parabola that is rotated about its origin. The dish has a focal length f 206 measured from a point 213 at the center of the circular upper area of the dish along the central axis, to a collection region 207 at the surface of the dish. In one embodiment, the paraboloid collector module 200 is designed to have the radius r 201 of its circular rim 211 be exactly equal to the focal length 206 of the dish, but in other embodiments it is possible that the radius of the circular rim does not necessarily have to be equal to the focal length. Such a structure can be easily manufactured by casting from a single paraboidal mold. Alternatively, a large array of them arranged in the shape of the designed collector array 100 of FIG. 1A could be made in a single mold. The thickness t 208 of the wall of the collector module 200 may be minimized for any specific material out of which the module is made, subject to certain trade-offs mentioned below. For polymeric glass materials, such as poly-methyl-methacrylate (PMMA), also known as acrylic glass, it can be as thin as a few millimeters. The exact thickness can be chosen as an engineering trade-off between mechanical robustness and the weight of a single collector module (or array of modules). If it is too thin, it could be susceptible to damage from handling or ambient turbulence, but if it is too thick and therefore heavy, it could contribute too much weight to the total weight of the collector array 100. The total weight of the collector array 100 should directly balance a need for structural robustness and a requirement for low power for operating the tracking systems that control the alignment and pointing of the array 100 to the optimum position of the sun. For an array made from acrylic glass material, a thickness of 1 mm for the module material would be ideal; this would result in the weight of a single, completely sealed collector module being 41.56 grams if the external rim diameter is 15 cm, and its internal rim diameter is 14.9 cm. For this illustrative example, we have taken the radius of the module to be equal to its focal length. The weight of 64 such collector modules would be about 2.66 kg (assuming a density of 1.18 grams/cm³ for PMMA).

While a paraboloid collector module 200 is described herein, it will readily be appreciated that different shapes may be utilized. What is required is a collector module that is capable of receiving solar radiation, with optical components that guide the solar radiation to a light receiver in the form of an optical-fiber. In the present embodiment, a concave collection surface is provided which is reflective and which is configured to collect sun rays and to reflect them towards a location at which a mirror is mounted. The mirror receives sun rays reflected from the collection surface and redirects them to a light collection point where a light receiver such as an optical-fiber can be coupled. Any shape that satisfies these criteria, with any suitable optical guiding components may be utilized in accordance with the principles described herein.

In the embodiment described herein the solar collector apparatus comprises collector modules that utilize reflection to collect and guide the sunlight onto the light receiver. Once the principle of separately harvesting the sunlight at a collection location, and guiding it using optical fibers to a utilization location are understood it will readily be appreciated that other alternatives may be available for collecting the sunlight. For example, sunlight may be collected using refractive rather than reflective optics. Refractive optics involves use of lenses alone. It would be possible to use arrays of convex lenses or Fresnel lenses to focus the light to a point where a fiber can be placed to capture it. Having said that, there may be advantages to utilizing reflective optics. Achieving the right precision on a large array of lenses involved in refractive optics may be harder than achieving the same precision using mirrors. Furthermore, some lenses have a defect called ‘chromatic’ aberration that may be unavoidable, while mirrors do not suffer from this. Another important consideration is weight. Conventional lenses need to have a thickness to refract light, which adds weight. A mirror on the other hand may be as thin as required. Unless, however, the lens is a meta-lens, which may be comprised of microscopically engineered surface features that permit fabrication of a flat lens for focusing of a certain wavelength band; full spectrum meta-lenses are still challenging to fabricate.

To enhance proper functioning, the concave inner lining of each module 200 in the collector array 100 should desirably be coated with a broadband high reflectivity film 209 or stack of films. The reflectivity for the inner lining 209 for each module 200 in the array should be 100% for sunlight wavelengths spanning the spectral range from 350 nm to 2500 nm. Most energy (about 95%) from the sun reaching the earth is concentrated within this spectral band. The energy is distributed non-uniformly in the solar spectrum. It is estimated that about 4% is contained between 300 nm and 400 nm; 42% between 400 nm and 700 nm, and 52% between 700 nm and 2500 nm. In a fully assembled collector array, each module 200 in the array has a thin transparent glass cover 203 extending over the open area defined by the rim 211 of the dish; this may be made from lightweight, durable, and ultraviolet-resistant plastic material. The cover 203 serves the dual role of protecting the concave inner lining 209 of the module from the elements as well as acting as an input port for parallel incident solar radiation rays 204 and 205 into the collector module. Solar radiation rays, such as 204 and 205, are reflected from the inner lining 209 and, because of the particular parabolic curvature of the module, redirected toward the focal point 213 of each dish in the vicinity of the center of the cover glass. A perfect hyperboloid mirror reflector 202, attached to the center of the cover 203 and positioned in the vicinity of the dish focal point, retro-reflects and refocuses the light to the bottom of the dish to the collection region 207, below which is attached a fiber-optic waveguide 210 with an appropriate numerical aperture. Here, numerical aperture is defined as a dimensionless parameter that characterizes the range of angles of incident light rays that are successfully captured by the fiber and are thus readily transported along its length.

The fiber-optic waveguide 210 may be attached by any suitable mechanism. In one embodiment, a screw thread around a ferrule can be created at the fiber tip 230, and a corresponding threaded body 232 can be provided at the collection point 207 of the collector module such that the tip 230 strand of the fiber-optic can be screwed into the threaded region at the bottom of the module. Technology for securing optical-fibers to curved and planar surfaces is known and may be adapted for use herein.

The fiber-optic waveguide 210 may have a circular cross-section core waveguide 234 whose diameter may range from 100 microns to 1 millimeter and whose cladding thickness can range between 150 microns and 1 millimeter. It will readily be appreciated that other dimensions may also be appropriate, depending on the context. In some examples, a fiber-optic waveguide for a single collector module could be capable of transporting a minimum of 10 W of sunlight for a distance of at least 1 km with minimal loss (<10 dB/km) over most of the spectral band in which the majority of solar energy is contained. Greater distances may be enabled depending on the context. Over the majority of the spectrum, the loss should be below 5 dB/km. For good performance and to maximize efficiency, the fiber-optic waveguides 210 should exhibit broadband transmission of sunlight beginning from the wavelength of 350 nm and ending at the wavelength of 2500 nm. The inventor has recognized certain spectral features of sunlight when considering the transportation requirements which have not hitherto been studied in depth; they have recognized that it is desirable that the sunlight transmission capability of the fiber between the wavelengths of 350 nm and 450 nm be greater than 20%, and between 450 nm and 700 nm, it should be greater than 85%, and between 700 nm and 1700 nm it should be 90% or greater, except for a narrow band of about 20 nm centered around the atmospheric water vapor absorption line at the wavelength of 1430 nm, where the transmission may dip to almost zero. This dip is of no consequence because there is little to no incident solar radiation at this wavelength due to atmospheric absorption of sunlight. The inventor has recognized that this is because the same absorption mechanisms (water molecules and hydroxyl ions) in the atmosphere are also present in the manufacture of glass fibers (from humidity in the air). Between the wavelengths of 1450 nm and 1900 nm, the fiber transmission should preferably be greater than 85%, and between 1900 nm and 2000 nm, it should preferably be better than 30%. For the remainder of the solar spectrum between 2000 nm and 2500 nm, the fiber transmission is expected to be between 15% and 20%. Low transmission in the last spectral region should not be a problem because the amount of solar energy carried in this portion of the spectrum is less than 1%. What is important is that the spectral transmission characteristic of the fiber should closely follow the distribution of solar energy reaching the earth as described above. This means that where there are dips in the solar energy spectrum reaching earth, the fiber may have similar dips in transmission since there is little energy to transmit. Overall, however, the delivery of sunlight through a fiber-optic waveguide should incur very little loss of light, certainly no more than 10 dB/km at worst but below 5 dB/km at best, over the spectral band in which most solar energy is contained.

There are a number of possible uses of sunlight transported in the manner described above. In the following, it is utilized in a light collection housing to provide an illumination zone that may have different purposes. Reference will now be made to FIGS. 2A, 2B, 2C, 2D and 2E to describe a method and architecture for electricity generation which enables simple replacement of photovoltaic cells.

This approach removes constraints of existing photovoltaic panels which integrate the sunlight gathering surface onto the conversion substrate, making it impossible to contemplate other uses of the collected sunlight or replacing any of the components when it is technically necessary.

FIG. 2A shows a light cabinet 311 from a side view with a plurality of racks 300 vertically spaced within the light cabinet 311, each containing rack mountings 312 and 313 vertically spaced within the rack 300. There could be one or more light cabinets 311 in a special shed or room inside a building where solar energy is converted to electricity. The ends of the ‘super’ fiber-optic cables 413 remote from the collector array(s) are received by respective intakes 301. In this way the ‘super’ fiber-optic cables 413, transporting sunlight, enter the light cabinet 311 and are distributed among the various racks 300 contained therein. As shown in FIG. 2A, these may be an intake 301 per rack 300, but other configurations are possible. Each rack mounting 312 is provided with an excess cable cradle 302 to take up any slack that might be necessary. In entering the rack 300, each ‘super’ fiber-optic cable is separated into at least two fiber-optic cables 401. The incoming fiber-optic cables 401 housed in the ‘super’ fiber-optic cables 413 are guided towards light boxes 304. Each rack mounting 312 may have one or more light boxes; five per mounting 312 are shown in FIG. 2B by way of example. Each optic-fiber cable 401 terminates at a ferrule 409 that guides the fibers into the light box 304. This is shown in expanded view 400. In the example given, each light box 304 takes the form of a container with four side walls, two of which are denoted 411A, 411B, an upper surface 402 and a lower surface 414; the box receives fibers from one or more cables. The fibers are delivered individually into point guides 410 arranged in a rectangular m x n matrix format (m<n) on either side wall of the light box. This is shown in FIG. 2C. Each light box 304 is aligned on top of a solar cell chip 405 inside a drawer 406. The number of fibers depends on how large each solar chip is and how much electrical power one wants to generate from the chip. Since this is a question for how much capacity a user wants, it may be specified as a design parameter. At a possible minimum, each light box over a chip can generate up to 1 kW. This may be translated to either 100 fiber strands which provides up to 1000W where each fiber carries 10W, or 64 fibers where each fiber caries 20W per fiber to give a total of 1280W, routed to each light box. Other configurations are possible. The preceding examples are given by way of illustration only.

Details of how the light box interfaces with the solar cell chip are shown in the expanded view 400 of FIG. 2C. Each fiber waveguide 210 in the fiber-optic cable 401 is fed through a ferrule 409 acting as a point guide in the wall that guides it into light box 304. The external side walls of the box should preferably be made from optically opaque materials such as anodized aluminum. In the detailed illustration in FIG. 2D, the interior of the box 304 is a specially designed cavity 110 into which each fiber 210 delivers its output beam 412. Special fiber terminators can be used at the tips of the fibers to obtain desired beam shapes within the cavity. In general, it is known that a fiber tip can be flat, lens-shaped, or any other desirable termination geometry for a particular exit beam shape. For the purposes of the light box, the desired fiber tip shape should result in an exit beam that is Gaussian. Most of the cavity 110 is empty space except for a triangular-shaped prism 403 whose two surfaces facing the fibers are covered with dielectric reflecting coatings. The angle of the inclined sides of the prism, with respect to the horizontal lower surface of the box, is chosen such that light incident onto them from the fibers is reflected downward toward a first microstructured optical diffuser 404. In the present embodiment, the illustrated angle α is 45°. Other angles may be utilized, for example in the range from 30° to 60°. The requirement is to redirect the incoming beams to overlap in an illumination zone. Beamlets such as designated by 412 from the fibers 210 should overlap at the edge of the first optical diffuser 404 because of diffraction at the exit of the fiber. To achieve this, the total distance, from the beam exit at the fiber 410 to the surface edge of the diffuser 404, should be chosen to guarantee beam overlap at the diffuser 404. A beam 412 a is shown overlapping the beam 412 in FIG. 2E. A second diffuser 408 may also be used if necessary, below the first diffuser 404. Because of the angular spread of light from each fiber 210, and the distance from the beam exit to the edge of the diffuser, the beams from the fibers overlap and mix just before they reach the first diffuser 404. During transmission through the first diffuser 404, the beams are randomly mixed by the action of the microstructure in the diffuser. Light emerges from the other side with a substantially uniform distribution. If there is a second diffuser 408, the microstructure on the second diffuser 408 further randomizes the light, thus enhancing uniform distribution. The apparatus is constructed so that the output is a beam that is substantially of uniform intensity distribution and shaped to fit precisely over the active surface of the solar chip 405. This implies that the output surface of the last diffuser should be sized to have the dimensions of the active area of the solar chip 405.

While this might typically be a square or rectangle (for ease of manufacture), any suitable geometric shape could be utilized. Indeed, it is not essential that there is a precise match between the output surface of the diffuser and the active area of the solar chip, but it will readily be understood that it is much more efficient in terms of usage of the sunlight which has been transported through the fibers if this is the case.

In another embodiment, the diffused light from the fiber-optic waveguides 210 may be used to illuminate a panel of photovoltaic cells, such as is currently in use in external environments for the conversion of solar energy to electricity. The advantage derived from use of the apparatus described herein is that such a panel may be utilized internally and therefore is not subject to environmental wear, as is currently the case. The current expectation is that illuminating photovoltaic panels of the known type may be less efficient than providing solar chips to capture the output of each light box, but that might not necessarily be the case.

Reverting back to the embodiment described herein, FIG. 2D shows an expanded perspective view of the light box and chip carrier of the embodiment described herein. This shows a rectangular output from the diffuser directly matching the solar cell chip underneath it on the chip carrier.

FIG. 2F illustrates a zoomed in section of FIG. 2D, showing one half of the arrangement in more detail. In an alternative embodiment, not shown, the prism may be replaced by a block of metal covered with a reflecting dielectric surface coating 116. This provides similar functionality to the prism, and may enable smaller light boxes to be constructed as they receive an array of light guides only from one side of the box.

The light incident on the first microstructured diffuser arrives there after being reflected from the only inclined surface in the cavity. As in the previous embodiment, the light is mixed and randomized, and when it emerges out of the second diffuser 408, it is uniformly distributed and can thus be projected on to a solar cell chip below it. As before, the dimensions of the diffusers are sized to match those of the active surface of the solar cell chip.

In a second embodiment, the light collection housing can be used to create a lamp with uniformly distributed light coming out of it. Such a lamp could be made from light-emitting diodes. Because of their small size, light-emitting diodes constitute point sources, emitting light that is diffracted in a similar fashion to that emanating from a fiber. Light-emitting diodes are installed at the positions where the fiber strands in the first embodiment are. The cavity functions exactly as described above. The output from the bottom diffuser would then be the output of a light-emitting diode ‘lamp’.

Reverting to the first embodiment, there follows a description of its use in association with a replaceable cell bank. As shown in FIG. 2D, and more clearly in FIG. 3, the solar cell chips 405 are mounted on a carrier 505 inside a chip drawer 406. For heat dissipation purposes, the drawer should be thermally conductive. It should have a casing 407 manufactured from oxide-free copper material because of its excellent thermal conductivity. Embedded within the copper casing block is a piping structure 511 that is used to circulate a coolant, such as chilled water, that transports away waste heat generated during operation of each solar cell. This may be necessary even in the best solar cell chips, if an unacceptably high fraction of incident sunlight is converted to heat, which would tend to degrade the performance of the conversion process.

FIG. 3 shows the details of the structure of an apparatus on a typical rack mounting 313 in a typical rack 300 of Figure. 2A. An assembled active conversion package 500 in FIG. 3 is comprised of the ‘super’ optic-fiber cable 413 that is separated into optic-fiber cables 401 that are fed into ferrules 409 that guide them into each light box 304, which interfaces with the cell drawer 406. Reference numeral 105 denotes a wheel/roller mechanism for rolling the drawer in and out. The cell drawer 406 is comprised of a copper block casing 407 on which is mounted a ceramic chip carrier 505 on top of which the solar cell chips 405 are attached and bonded by gold wires 507. The drawer 406 has a handle 106 so that it may be easily slid out from the rack. To manufacture the assembly, a ceramic chip carrier initially is covered with a thin layer of highly conducting metal (such as gold); this layer is then lithographically defined into separate regions that are electrically isolated. These isolated regions are in turn defined into two electrical regions: one negative and the other positive. A negative terminal 508 and a positive terminal 509 are attached between which the solar cell chip 405 is mounted. Bypass diodes 510 protect each solar chip from any potential excess and uncontrollable current generation process by short-circuiting the chip to ground in the event of such an occurrence.

As shown in FIG. 4, embedded inside the copper block 407 on which the ceramic solar chip carrier 505 sits is a winding pipe 511 that allows a cooling fluid, such as ethylene glycol diluted with water or pure water, to be flowed and taken out at outlet 513. Such a cooling system can be closed loop. After exiting port 513, the coolant can then be fed into an associated heat exchanger before it is fed back into the copper block at an inlet port 512.

FIG. 5 illustrates details of the drawer comprising the copper block into which the ceramic chip carrier is installed. To make it easy to replace the bank of solar cell chips mounted on the carrier, each edge of the carrier is machined into a tongue 600 that fits into a slot 606 in the copper block 407. Once installed in the block, the carrier can be secured in place using latches 604 on the right and left side of the copper block carrying the ceramic carrier. Whenever necessary, the carrier can be removed by simply unlatching the mechanism and pulling it out. The carrier and the block should make intimate contact with each other to facilitate thermal conduction. Heat transferred to the block from the carrier is transported away by the coolant described above with reference to FIG. 4.

A ceramic carrier populated with a bank of solar cell chips is shown in FIG. 6. As discussed, each solar cell chip on the carrier is protected with bypass diodes in case of excessive electrical current. Electrical output from the solar cell chips is available from the positive and negative terminals 508 and 509, respectively. Wire bonds 507 on two sides of the cell and a thermally and electrically conductive paste on the bottom side of the cell attach the p and n side of the solar cell diode to an appropriate output terminal. Also, as described earlier, the tongue 600 on each side of the ceramic carrier slots into the copper block 407 that serves as a heat sink.

Some of the advantages of the scheme described in this invention should now be apparent to those skilled in the art. By separating the function of light collection from light transport, and the light collection process from the conversion process, one effectively makes the photovoltaic system future-proof. Technology advances and developments that impact performance improvements in new solar cell chips can be readily taken advantage of All that is required is removal of the old cell bank 514 on which solar cells are carried. New chip carriers (with new solar cells of higher performance) can then be readily swapped in to replace the old ones. FIG. 6 identifies a replaceable structure in the form of cell bank 514. The cell bank is the complete replaceable unit which comprises the carrier base 505, the cells 405 and the surrounding feature sets such as the diodes 510, wire bonds 507 etc. The cell bank can be slotted in and out of the casing 407 for replacement purposes once the casing has been removed from the rack, for example by sliding or rolling it out using the handle.

For owners of installed systems, this is a less expensive option than replacing an entire infrastructure. This partial replacement option is available to both utility scale power plants and to individual home photovoltaic systems. Another advantage of the new general methodology is that it allows a relatively straightforward process for increasing generating capacity of existing power plants. If desired, several empty solar chip storage racks, earmarked for future capacity expansion can be included during the initial installation phase. The empty racks can be populated with solar cell chip carriers at a later date when additional capacity is needed or when funds become available. This unmatched flexibility to scale up or scale down could give large, renewable solar energy utility plant operators decided advantages over their competitors who rely on traditional coal or gas plants. 

1. A method for collecting light at a housing adapted to receive light from a plurality of point light sources; the method comprising: receiving light beams from a plurality of light sources via at least one light transmissive region; securing the light sources relative to the housing with a securing means to direct their respective beams through the light transmissive regions into the housing; and guiding the beams into overlap at an exit region of the housing to form an illumination zone of substantially uniform intensity distribution.
 2. A method according to claim 1 comprising receiving the beams from the light sources at an inclined reflecting surface arranged to reflect them to the illumination zone in overlap.
 3. A method according to claim 2 comprising reflecting the beams from the reflecting surface in overlap toward at least one microstructured diffuser at the illumination zone, wherein the microstructured diffuser is adapted to spread the received light with a substantially uniform intensity distribution over an area with a defined geometrical shape.
 4. A method according to claim 1 wherein the securing means is configured to secure the light sources in one or more arrays.
 5. A method according to claim 2 comprising receiving the beams from two sets of light sources secured at opposite walls of the housing at two inclined reflecting surfaces that reflect them in overlap to the illumination zone.
 6. A method according to claim 2 wherein the angle of the inclined reflective surface with respect to the horizontal lower surface of the housing is 30° to 60°, optionally 45°.
 7. A method according to claim 1 comprising receiving the light beams from terminal ends of optical fibers.
 8. A method according to claim 1 comprising receiving the light beams from light-emitting diodes.
 9. A method according to claim 1 comprising directing the light of uniform intensity and defined geometrical shape exiting the microstructured diffuser at a photovoltaic component of the same geometrical shape 